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Searching for Quantum Gravity using Gamma Ray Bursts Frederick Kuehn Richard Hughes, Brian Winer Great Lakes Cosmology Workshop 8 June 1 2007 The Large Area Telescope Collaboration • The mission is a NASA/DOE and international effort • United States • California State University at Sonoma • UC Santa Cruz - Santa Cruz Institute of Particle Physics • Goddard Space Flight Center - Laboratory for High Energy Astrophysics • Naval Research Laboratory • The Ohio State University Some members of • Stanford University (SLAC and HEPL/Physics) the LAT collaboration • University of Washington • Washington University in St. Louis • France • IN2P3, CEA/Saclay • Italy • INFN, ASI • Japan • Hiroshima University PI: Peter Michelson (Stanford & SLAC) • ISAS, RIKEN ~ 250 members • Sweden Managed at the Stanford Linear • Royal Institute of Technology (KTH) Accelerator Center • Stockholm University Frederick Kuehn GLCW 08 June 1 2007 2 The LAT sits on top The GBM is distributed around the observatory About GLAST • Set to launch in late December • GLAST will observe a broad energy range with superior acceptance and resolution than previous instruments • LAT: 20 MeV - >300 GeV • GBM: 8 keV - 25 MeV • Looking in new energy regimes leads to unexpected discoveries 3 Frederick Kuehn GLCW 08 June 1 2007 Credit: NASA and General Dynamics Lorentz violation and the speed of light • Why test the constancy of the speed of light? • • • • One of the fundamental constants of physics Its constant speed is a requirement in relativity Also a requirement in quantum field theories Quantum Gravity: the long sought after unification of gravity with quantum mechanics is poorly understood and may include Lorentz invariance violation • No shortage theoretical ideas that produce deviations from c = constant • • • • • • • ‘Foamy’ nature of space time acts as a refractive index - gr-qg/0312044 ‘Doubly Special’ Relativity keeps L.I. but changes c - gr-qg/0207085 Lorentz violating SUSY - hep-ph/0505029 Loop Quantum Gravity - gr-qg/9403008 Spontaneous symmetry breaking in string theory - hep-th/0012060 Canonically quantized gravity involves Lorentz violation - gr-qc/9901023 ... see the review by Mattingly for more - gr-qc/0502097 Frederick Kuehn GLCW 08 June 1 2007 4 Some mathematical details • Usual assumption is that the L.I. dispersion is modified E2 = m2 + p2 → E2 = F(p,m) • Since the world is apparently nearly L.I. we Taylor expand the dispersion relation in the CMB rest frame (where p = 0 for a massive particle, or in the frame where the CMB energies is equal to its momentum) E2 = m2 + p2 + Fi(1)pi + Fij(2)pipj + Fijk(3)pipjpk + ... E2 = m2 + p2 + EPlfi(1)pi + fij(2)pipi + fij(3)pipjpk/EPl + ... • Usual assumptions about the expansion parameters • EPl ~ 1019 GeV (the scale at which we expect to see new physics) • We preserve rotational invariance, but break boost invariance: E2 = m2 + p2 + EPlf(1)|p| + f(2)p2 + f(3)|p|3/EPl + ... ❖ The f(3)|p|3/EPl term is relevant for astrophysical tests • The first two terms modify low energy behaviour, whereas the fourth and higher order terms do not provide measurable speed differences Frederick Kuehn GLCW 08 June 1 2007 5 Current bounds for one analysis • Modified dispersion relation leads to an energy dependent speed of light • In one case, the velocity is lower at high energies • v ≈ c[1 - ξ(E/EPL)] ❖ Δt ≈ ξ (ΔE/EPL) x (L/c) ~ ξ (ΔE/EPL) x H0-1 ∫dz/h(z) • ξ = f(3) in previous notation • Gamma Ray Bursts produce short intense flares over 7+ orders of magnitude of energy • By performing a time of flight measurement we can place limits on the speed of light at various energies ❖ We look for a systematic differences in arrival times of photons at different energies proportional to distance • Current GRB observations limited to limited to lower energy regimes (BATSE, BeppoSAX, HETE, SWIFT energies), hence the time delays will be small leading to to limits of EPL ≥ a few x 1016 GeV (e.g. astro-ph/0310307) • TeV observations by Milagro lead to similar bounds (astro-ph/9810044) Frederick Kuehn GLCW 08 June 1 2007 6 The impact of GLAST data • Here the arrival time for photons from a GRB with five pulses is shown • The GRB was placed at z~1 • mean redshift ~ 2 • In black we see the arrival times if there is no QG effect If we see no delay EPL > (L⋅ΔE)/(c⋅Δt) If we see a delay EPL = (L⋅ΔE)/(c⋅Δt) Naive energy scale that GLAST can probe (L⋅ΔE)/(c⋅Δt) = (1028cm)(102GeV)/(1010cm)(10-4s) = 1024 GeV • In green, the arrival times if EPL~1018 GeV • In red, the arrival times if EPL~1019 GeV • The LAT will be able to make this measurement assuming no fine tuning of expansion parameters Frederick Kuehn GLCW 08 June 1 2007 7 Conveniences and inconveniences ✓GRB pulses become narrower at ‘high’ energies ✓If the trend hold at LAT energies this will be very helpful for the determination of bounds on EPL ๏ GRBs are distant, poorly understood objects ๏ It is possible that for one burst the high energy emission is systematically delayed which would cause a fake signal for that burst ๏ Most analyses use single (very bright) bursts, to make the measurements (e.g. astro-ph/0610571) ❖ Looking for consistency between bursts with redshift measurements presents a way around this problem (e.g. astro-ph/0510172) • The effect should be correlated linearly with distance • All astrophysical objects (e.g.) AGN flares should show the same effects ❖ At OSU we are developing our own systematic analysis of multiple bursts to determine whether or not the effect is present in LAT data with statistical accuracy Frederick Kuehn GLCW 08 June 1 2007 8 Higher order effects • What if the time delay is proportional to energy to some power? Δt = (L/c)(a⋅E/EPL)b Phys. Rev. Lett. 83, 11, 1999 Milagro collaboration • Here we get a feeling for the sensitivity of time delay measurements to the QG scale as a function of the power law index • We are basically insensitive to higher order corrections Frederick Kuehn GLCW 08 June 1 2007 9 Conclusions • Physics at the Plank scale is inherently interesting, yet difficult to test and model • By measuring the speed of light at high and low(er) energies, GLAST will be able to set stringent limits on, or discover the effects of Quantum Gravity and Lorentz Invariance violation • Even with a clear signal from GRBs, a discovery of this magnitude would require extensive cross checks from other astrophysical phenomena Frederick Kuehn GLCW 08 June 1 2007 10